Haag's Theorem: Explain Free Field Nature

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SUMMARY

Haag's theorem establishes that free fields and interacting fields exist in different, unitarily inequivalent Hilbert spaces, meaning one cannot transform into the other. The theorem highlights the mathematical ill-definition of transitioning from a free to an interacting field due to infrared divergences. For a deeper understanding, refer to A. Duncan's book, "The Conceptual Framework of Quantum Field Theory," specifically section 10.5. Alternative approaches, such as the algebraic approach to quantum field theory (QFT), effectively address the challenges posed by Haag's theorem.

PREREQUISITES
  • Understanding of Haag's theorem in quantum field theory
  • Familiarity with Hilbert spaces and their properties
  • Knowledge of perturbation theory in quantum mechanics
  • Basic concepts of the algebraic approach to quantum field theory
NEXT STEPS
  • Study the algebraic approach to quantum field theory
  • Read A. Duncan's "The Conceptual Framework of Quantum Field Theory"
  • Explore the implications of infrared divergences in quantum field theory
  • Investigate unitarily inequivalent representations in quantum mechanics
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Physicists, quantum field theorists, and advanced students seeking to understand the implications of Haag's theorem and alternative modeling approaches in quantum field theory.

lindberg
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Can someone explain in simple terms why, according to Haag's theorem, a free field cannot become an interacting one?
What is the main reason for a free field staying free according to Haag's theorem?
 
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The formal transformation from a free to an interacting field turns out to be mathematically ill defined due to an IR divergence (infinite volume in which the fields live). For details, I highly recommend the book A. Duncan, The Conceptual Framework of Quantum Field Theory, section 10.5 How to stop worrying about Haag's theorem.
 
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lindberg said:
according to Haag's theorem, a free field cannot become an interacting one?
That's not quite what Haag's theorem says. A free field and an interacting field are different things, and one cannot "become" the other, regardless of what Haag's theorem or any other mathematical result says.

Haag's theorem says, basically, that free fields and interacting fields live in different, unitarily inequivalent Hilbert spaces. To someone who is used to the usual way of modeling interacting fields as perturbations of free fields, this seems like a problem; but there are other approaches to quantum field theory, such as the algebraic approach, in which it is not a problem at all.
 
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PeterDonis said:
To someone who is used to the usual way of modeling interacting fields as perturbations of free fields, this seems like a problem; but there are other approaches to quantum field theory, such as the algebraic approach, in which it is not a problem at all.
Wasn't Haag's conclusion extended later to other approaches?
I might be wrong, don't hesitate to correct me.

An Algebraic Version of Haag’s Theorem​

https://link.springer.com/article/10.1007/s00220-011-1236-7
 
lindberg said:
Wasn't Haag's conclusion extended later to other approaches?
Given that the whole point of the algebraic approach to QFT is to be able to deal with unitarily inequivalent representations, showing that the algebraic approach leads to unitarily inequivalent representations isn't much of an issue.
 
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